CN212932973U - Proton absolute energy spectrum measuring device - Google Patents
Proton absolute energy spectrum measuring device Download PDFInfo
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- CN212932973U CN212932973U CN202021054657.3U CN202021054657U CN212932973U CN 212932973 U CN212932973 U CN 212932973U CN 202021054657 U CN202021054657 U CN 202021054657U CN 212932973 U CN212932973 U CN 212932973U
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Abstract
The utility model discloses an absolute energy spectrum measuring device of proton. The proton absolute energy spectrum measuring device comprises: the Thomson ion spectrometer and the radiochromic membrane stack are sequentially arranged from the aiming laser emission end to the experimental target end; a central through hole is formed in the center of the radiation color-changing membrane stack; the axis of the central through hole is superposed with the axis of an inlet and an outlet of the Thomson ion spectrometer; the Thomson ion spectrometer is used for receiving aiming laser and enabling the laser to pass through a central through hole of the radiochromic membrane stack to reach an experimental target point; the experimental target is used for receiving experimental targeting laser and accelerating the experimental targeting laser to generate protons, the protons generated by the laser acceleration can irradiate on the radiochromic membrane stack to realize discrete energy angle distribution measurement, and a small part of the protons pass through a central through hole of the radiochromic membrane stack and enter a Thomson ion spectrometer to realize energy spectrum measurement. The utility model discloses synthesize this two sets of equipment of thomson ion spectrometer and radiochromic diaphragm stack and can realize the high accuracy energy spectrum measurement under the wide range.
Description
Technical Field
The utility model relates to a plasma physics and nuclear detection technical field especially relate to an absolute energy spectrum measuring device of proton.
Background
In laser ion acceleration studies, absolute measurement of proton spectra is crucial to understanding the physical process of laser-target interaction. The absolute measurement of proton energy spectrum is also the most comprehensive measurement of proton parameters. At present, the thomson ion spectrometer is mainly adopted for the diagnosis of proton energy spectrum. The thomson spectrometer is preceded by a collimating aperture (typically only tens to hundreds of μm in diameter), the size of which determines the spectral resolution of the ion diagnosis. It can only give a proton spectrum over a small spatial solid angle.
In order to obtain a wider range of energy spectral distribution studies, wide-angle proton spectrometers have also been developed. For example, using a collimating slit instead of a collimating aperture, a one-dimensional angular distribution of the proton energy spectrum can be obtained. However, due to the non-uniformity of the spatial distribution of protons, the measurement of such a one-dimensional angular distribution does not completely reflect the absolute spectral information. For example, proton angular distribution information of discrete energies can be obtained using a stack of stacked Radiochromic film (RCF) membranes. However, this method cannot provide continuous energy spectrum information, and the accuracy of the measured energy spectrum is worse than that of a thomson ion spectrometer due to the superposition of proton energy deposits. Therefore, the existing proton energy spectrum measurement has the problem of poor accuracy of wide-range energy spectrum measurement.
Disclosure of Invention
Based on this, it is necessary to provide a proton absolute spectrum measuring apparatus to realize high-precision spectrum measurement in a wide range.
In order to achieve the above object, the utility model provides a following scheme:
a proton absolute energy spectrum measuring apparatus comprising: the Thomson ion spectrometer and the radiochromic membrane stack are sequentially arranged from the aiming laser emission end to the experimental target end; the center of the radiation color-changing membrane stack is provided with a central through hole; the axis of the central through hole is superposed with the axis of an inlet and outlet hole of the Thomson ion spectrometer; the Thomson ion spectrometer is used for receiving aiming laser and enabling the aiming laser to pass through a central through hole of the radiochromic membrane stack to reach an experimental target point; the experimental target is used for receiving experimental targeting laser and accelerating the experimental targeting laser to generate protons, and the protons are irradiated on the radiochromic membrane stack; the thomson ion spectrometer is also configured to receive protons that pass through a central through-hole of the radiochromic membrane stack.
Optionally, the thomson ion spectrometer includes an imaging plate, a spectrometer electromagnetic assembly and a spectrometer collimator, which are sequentially disposed from the targeting laser emission end to the experimental target end; the imaging plate and the spectrometer collimator are both connected with the spectrometer electromagnetic assembly; a first collimating hole is formed in the center of the spectrometer collimator; the axis of the central through hole coincides with the axis of the first collimating hole.
Optionally, the radiochromic membrane stack includes a radiochromic membrane set and a metal shielding membrane stacked in a horizontal direction; the radiochromic diaphragm set comprises a plurality of layers of first radiochromic diaphragms which are stacked along the horizontal direction; the metal shielding diaphragm is arranged on one side far away from the Thomson ion spectrometer.
Optionally, the diameter of the central through hole is larger than the diameter of the first collimating hole.
Optionally, the thomson ion spectrometer further comprises a second radiochromic membrane; the second radiochromic diaphragm is arranged at the front end of the spectrometer collimator and is positioned between the Thomson ion spectrometer and the radiochromic diaphragm stack; a diaphragm through hole is formed in the center of the second radiochromic diaphragm; the diameter of the diaphragm through hole is larger than that of the first collimating hole.
Optionally, the proton absolute energy spectrum measuring apparatus further includes an aiming laser pen; the aiming laser pen is used for emitting the aiming laser and enabling the aiming laser to enter the Thomson ion spectrometer.
Optionally, the proton absolute energy spectrum measuring apparatus further includes a first adjusting platform, a second adjusting platform, and a third adjusting platform; the Thomson ion spectrometer is arranged on the first adjusting platform, and the first adjusting platform is used for adjusting the lifting, the transverse translation, the rotation and the pitching of the Thomson ion spectrometer; the radiochromic membrane stack is arranged on the second adjusting platform, and the second adjusting platform is used for adjusting the translation and the lifting of the radiochromic membrane stack; the aiming laser pen is arranged on the third adjusting platform; and the third adjusting platform is used for adjusting the position of the aiming laser pen.
Optionally, the proton absolute energy spectrum measuring device further includes an organic glass collimator; a second collimating hole is formed in the center of the organic glass collimator; the organic glass collimator is used for replacing the spectrometer collimator when aiming operation is carried out.
Optionally, the proton absolute energy spectrum measuring apparatus further includes a collimator plate; the aiming piece is arranged at an experimental target point; the distance between the sighting piece and the radiochromic membrane stack is 5cm-10 cm.
Compared with the prior art, the beneficial effects of the utility model are that:
the utility model provides an absolute energy spectrum measuring device of proton, this absolute energy spectrum measuring device of proton includes: the Thomson ion spectrometer and the radiochromic membrane stack are sequentially arranged from the aiming laser emission end to the experimental target end; a central through hole is formed in the center of the radiation color-changing membrane stack; the axis of the central through hole coincides with the axis of the inlet and outlet holes of the Thomson ion spectrometer. The utility model discloses combine Thomson ion spectrometer and radiochromic diaphragm stack, given the absolute energy spectrum that is higher than certain energy laser acceleration proton, realized the high accuracy energy spectrum measurement under the wide range.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings required to be used in the embodiments will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to these drawings without inventive labor.
Fig. 1 is a schematic structural diagram of a proton absolute energy spectrum measuring apparatus according to an embodiment of the present invention;
fig. 2 is a flowchart of a method for aiming a proton absolute energy spectrum measuring device according to an embodiment of the present invention.
Detailed Description
The technical solutions in the embodiments of the present invention will be described clearly and completely with reference to the accompanying drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only some embodiments of the present invention, not all embodiments. Based on the embodiments in the present invention, all other embodiments obtained by a person skilled in the art without creative work belong to the protection scope of the present invention.
In order to make the above objects, features and advantages of the present invention more comprehensible, the present invention is described in detail with reference to the accompanying drawings and the detailed description.
Fig. 1 is a schematic structural diagram of a proton absolute energy spectrum measuring device according to an embodiment of the present invention.
Referring to fig. 1, the proton absolute energy spectrum measuring apparatus of the present embodiment includes: a Thomson ion spectrometer and a radiochromic diaphragm (RCF) stack which are sequentially arranged from the aiming laser emission end to the experimental target end; the center of the radiation color-changing membrane stack is provided with a central through hole; the axis of the central through hole is superposed with the axis of an inlet and outlet hole of the Thomson ion spectrometer; the Thomson ion spectrometer is used for receiving laser and enabling the laser to pass through a central through hole of the radiochromic membrane stack to reach an experimental target point; the experimental target is used for receiving experimental targeting laser and accelerating the experimental targeting laser to generate protons, and the protons are irradiated on the radiochromic membrane stack; the thomson ion spectrometer is also configured to receive protons that pass through a central through-hole of the radiochromic membrane stack.
The indoor target laser generator that is provided with of target in this embodiment, the laser that target laser generator sent beats as experiment targeting laser on the actual target of experiment target point department, actual target absorbs experiment targeting laser makes experiment targeting laser is accelerated to produce proton and can irradiate and be in realize discrete energy angular distribution on the radiochromic diaphragm stack and measure. Wherein a small portion of protons will pass through the central through hole of the radiochromic membrane stack into the thomson ion spectrometer enabling recording of a continuous proton spectrum for a given small spatial solid angle. By integrating two sets of equipment, namely a Thomson ion spectrometer and a radiochromic diaphragm stack, high-precision energy spectrum measurement in a wide range is realized.
As an optional implementation manner, the thomson ion spectrometer includes an imaging plate 1, a spectrometer electromagnetic assembly 2 and a spectrometer collimator 3, which are sequentially arranged from the aiming laser emission end to the experimental target end; the imaging plate 1 and the spectrometer collimator 3 are both connected with the spectrometer electromagnetic assembly 2; a first collimating hole is formed in the center of the spectrometer collimator 3; the axis of the central through hole is superposed with the axis of the first collimating hole; the diameter of the central through hole is larger than that of the first collimating hole. The diameter of the first collimating holes may be 0.1mm to 0.5 mm. The spectrometer collimator 3 may be made of a tantalum metal material.
As an alternative embodiment, the diameter of the first collimating aperture is 0.2 mm.
As an alternative embodiment, the radiochromic membrane stack comprises a membrane set 4 and a fixture frame 5; the membrane group 4 is mounted in the jig frame 5. The membrane group 4 comprises a radiochromic membrane group and a metal shielding membrane which are stacked along the horizontal direction; the radiochromic diaphragm set comprises a plurality of layers of first radiochromic diaphragms which are closely stacked along the horizontal direction; the metal shielding diaphragm is arranged on one side far away from the Thomson ion spectrometer.
As an optional implementation mode, the metal shielding membrane and the multilayer first radiochromic membrane are square membranes which are cut to be 5cm-10cm wide, and a through hole with the width of 1mm-3mm is formed in the center. The cross section of the clamp frame 5 is square, the inner dimension width is 5cm-10cm, and the depth is 1cm-2 cm. The metal shielding diaphragm can be an Al diaphragm with the thickness of 25 microns, and the first radiochromic diaphragm can be a radiochromic diaphragm with the model of HD-V2.
As an alternative embodiment, the transverse dimensions of the metal shielding diaphragm and the multilayer first radiochromic diaphragm are both 5cm × 5cm, and a through hole with the thickness of 3mm is formed in the center. The inner dimension of the clamp frame 5 is 5cm × 5cm × 1 cm. The jig frame 5 may be an aluminum jig frame.
As an alternative embodiment, the thomson ion spectrometer further comprises a second radiochromic membrane 6; the second radiochromic diaphragm 6 is arranged at the front end of the spectrometer collimator 3 and is positioned between the thomson ion spectrometer and the radiochromic diaphragm stack; a diaphragm through hole is formed in the center of the second radiochromic diaphragm 6; the diameter of the diaphragm through hole is larger than that of the first collimating hole. The second radiochromic membrane 6 is tightly attached to the spectrometer collimator 3 during measurement, and the diameter of the membrane through hole is larger than that of the first collimating hole, so that protons can enter the first collimating hole. The second radiochromic film 6 can also be a radiochromic film with the model number HD-V2. The diameter of the diaphragm through hole may be 3 mm.
As an alternative embodiment, the proton absolute energy spectrum measuring device further comprises an aiming laser pen 7; the aiming laser pen 7 is used for emitting the aiming laser and enabling the aiming laser to enter the Thomson ion spectrometer.
As an alternative embodiment, the proton absolute energy spectrum measuring apparatus further includes a first adjusting platform 8, a second adjusting platform, and a third adjusting platform 9. The second adjusting platform comprises a supporting rod 10 and a two-dimensional adjusting platform 11, and the clamp frame 5 is installed on the supporting rod.
The thomson ion spectrometer is arranged on the first adjusting platform 8, and the first adjusting platform 8 is used for adjusting the position and the pointing direction of the thomson ion spectrometer, such as four-dimensional adjustment of lifting, transverse translation, rotation and pitching of the thomson ion spectrometer. The position adjusting range of the first adjusting platform 8 is +/-2 cm, and the adjusting precision is 10 micrometers; the angle adjusting range is +/-5 degrees, and the adjusting precision is 0.1 degree.
The radiochromic diaphragm stack is arranged on the second adjusting platform, and the second adjusting platform is used for adjusting the spatial position of the radiochromic diaphragm stack, for example, realizing the two-dimensional adjustment of translation and lifting of the radiochromic diaphragm stack. The translation adjusting range of the second adjusting platform is 0cm-20cm, the adjusting precision is 10 microns, the lifting adjusting range is +/-1 cm, and the adjusting precision is 10 microns. The support rod 10 may be a stainless steel support rod.
The aiming laser pen 7 is arranged on the third adjusting platform; the third adjusting platform 9 is used for adjusting the position of the aiming laser pointer 7. The aiming laser pen 7 emits green light with a divergence angle of less than 1mrad and a beam spot of less than 1 mm.
As an alternative embodiment, the proton absolute energy spectrum measuring device further comprises a plexiglass collimator; a second collimating hole is formed in the center of the organic glass collimator; the plexiglass collimator is used to replace the spectrometer collimator 3 when performing the aiming operation. The position and shape of the second collimating holes is the same as the position and shape of the spectrometer collimator 3. The diameter of the second collimating holes may be 1 mm.
As an optional embodiment, the proton absolute energy spectrum measuring device further comprises a sighting piece 12; the aiming block 12 has a flat surface, the position and angle of the aiming block 12 are consistent with those of an actual target, and the aiming block 12 can be arranged at an experimental target point. The distance between the sighting piece 12 and the radiochromic membrane stack is 5cm-10 cm. In particular, the distance between the aiming block 12 and the radiochromic membrane stack may be 5 cm.
As an alternative embodiment, the size of the aiming plate 12 is 1mm × 1mm, and the aiming plate 12 may be a Cu film with a thickness of 100 μm.
The proton absolute energy spectrum measuring device is realized by the following principle:
the proton absolute energy spectrum measuring device is used for diagnosing by combining the radiochromic membrane stack and the Thomson ion spectrometer, and protons generated by laser acceleration sequentially pass through the metal shielding membrane and the first radiochromic membranes of all layers. And part of protons passing through the central through hole of the radiochromic membrane stack sequentially pass through the first collimating hole of the Thomson ion spectrometer and the spectrometer electromagnetic assembly 2, and finally enter the imaging plate 1 to record proton signals. After receiving the protons passing through the central through hole of the radiochromic membrane stack, the thomson ion spectrometer obtains the absolute energy spectrum of the protons by the existing contrast analysis (statistical analysis method) and data fitting (polynomial fitting) methods built in the thomson ion spectrometer. The proton absolute energy spectrum measuring apparatus can be realized by a method which is not the only method that can be realized. It points out here that the utility model discloses only improve proton absolute energy spectrum measuring device, just can obtain the absolute energy spectrum according to proton absolute energy spectrum measuring device, as long as based on proton absolute energy spectrum measuring device, adopt with above-mentioned contrastive analysis and data fitting method the same or similar principle homoenergetic can obtain the absolute energy spectrum, specific implementation method does not limit here.
In practical applications, the proton energy deposit presents a bragg peak, i.e. its main energy deposit at the end of its range. And the energy deposition curve structure of the ions in the material is the same after normalization relative to the range of the ions. Let the normalized energy curve equation be f (x), (0< x <1, f (x) ≦ 1). The number of the first radiochromic diaphragms in the radiochromic diaphragm stack is N. With the 1 st plate facing the proton incident direction. And (4) counting the dose of RCF of each layer after the experiment is finished, wherein the counting comprises two types of counting.
(1) Counting the whole sheet dose, wherein the Bragg peak of the proton with the energy E (i) is positioned at the position of the ith layer of radiochromic film. The statistical dose of the i-th layer of radiochromic membrane is D (i), and the statistical dose corresponding to the energy E (i) corresponding to the i-th layer of radiochromic membrane is the statistical dose D (i) minus the dose deposition generated by the high-energy protons, namely
(2) And counting the dose on the radiochromic membrane which is close to the collimating hole and has the same area with the collimating hole. The statistical dosage of the ith layer is dD (i), and the statistical dosage corresponding to the energy E (i) corresponding to the ith layer of the radiochromic membrane is dD (i)
Dividing the statistical value in the step (1) by the statistical value in the step (2) to obtain the statistical value
Then the ratio of all the radiation color-changing films is counted to obtain the ratio D of discrete energyratio(E (i)) performing polynomial fitting on the statistical data to obtain a relation D of the ratio changing along with energyratio(E)。
The use of a Thomson spectrometer gives a through-collimated holeThe continuous energy spectrum distribution I (E) of the proton, so that the actual absolute energy spectrum distribution of the proton is Iabs(E)＝I(E)×Dratio(E)。
In the measurement, due to the large number of low-energy protons, the count of the first radiochromic membrane (even the second radiochromic membrane) may be saturated, so that the absolute energy spectrum of the low-energy protons cannot be given, but the absolute energy spectrum of the protons with higher energy can be given by the method.
In the measuring process, the distance between the radiochromic diaphragm stack and an experimental target point is about 5cm-10cm, and if the radiochromic diaphragm stack is directly placed in a diagnosis area (position) before measurement, the work of an aiming target system can be influenced. The radiochromic membrane stack is therefore moved out of the diagnostic position prior to measurement. And moving the radiochromic membrane stack to a diagnosis position when the formal targeting is to be measured. The diagnostic process thus involves an accurate reset of the radiochromic membrane stack. Poor positional reset accuracy of the radiochromic diaphragm stack may affect the signal acquisition of a subsequent thomson spectrometer. On the other hand, in the integrated package of the thomson ion spectrometer, a collimator is usually made of a heavy metal material with the thickness of several mm to 1cm, and a central collimating hole is only about hundreds of microns, so that the direct laser collimation is difficult. Before measurement, the following method for aiming the proton absolute spectrum measuring device can be adopted to perform the aiming operation on the proton absolute spectrum measuring device. Fig. 2 is a flowchart of a method for aiming a proton absolute energy spectrum measuring device according to an embodiment of the present invention.
Referring to fig. 2, the aiming method includes:
(1) determination of aiming light path
Before measurement, the spectrometer collimator 3 in the Thomson ion spectrometer is replaced by an organic glass collimator, namely, a collimation hole of the organic glass collimator is placed at the position of an actual collimation hole. The aiming laser pointer 7 is located behind the imaging plate 1 of the thomson spectrometer. The position of the aiming laser pen 7 is adjusted to enable the laser emitted by the aiming laser pen 7 to penetrate out from the center of a second collimating hole of the organic glass collimator and irradiate on the aiming plate 12, the circular diffraction light spot of the laser can be seen on the aiming plate 12, and the adjusted position of the aiming laser pen 7 is determined as the measuring position of the aiming laser pen, so that the determination of an aiming light path is realized.
(2) Determination of aiming angle
The position of the thomson ion spectrometer is adjusted, so that the laser returning from the aiming plate 12 returns to the second collimating hole in the original path, and the adjusted position of the thomson ion spectrometer is determined as the measurement position of the thomson ion spectrometer, namely, the determination of the aiming angle of the spectrometer is realized.
Through the two steps (1) and (2), the collimation of the Thomson ion spectrometer on the target normal can be realized, so that the diagnosis requirement of diagnosing the target back normal proton energy spectrum is met.
(3) Determination of diagnostic position of radiochromic membrane stack
Moving the radiochromic membrane stack into a diagnosis area, adjusting the position of the radiochromic membrane stack to enable the laser to penetrate out of a central through hole of the radiochromic membrane stack, then taking off the organic glass collimator, and replacing with an actual collimator, namely replacing the organic glass collimator with a spectrometer collimator 3. And adjusting the position of the radiochromic membrane stack at the moment, so that the laser penetrates out of the central through hole of the radiochromic membrane stack, and determining the adjusted position of the radiochromic membrane stack as the measuring position of the radiochromic membrane stack. The radiochromic membrane stack is then moved out of the diagnostic region.
(4) And (5) checking an actual experiment.
Fixing the second radiochromic membrane 6 at the front end of the spectrometer collimator 3, so that the axis of the membrane through hole of the second radiochromic membrane 6 coincides with the axis of the first collimating hole of the spectrometer collimator 3, i.e. the membrane through hole of the second radiochromic membrane 6 covers the first collimating hole of the spectrometer collimator 3.
And (3) sealing the target chamber, vacuumizing to enable the proton absolute energy spectrum measuring device to be in a vacuum environment, moving the radiochromic membrane stack into the radiochromic membrane stack measuring position, and when the second radiochromic membrane 6 changes color (when the position near a membrane through hole of the second radiochromic membrane 6 changes color), proving that protons can reach the first collimating hole through the radiochromic membrane stack, so that the aim of the proton absolute energy spectrum measuring device is realized, otherwise, the step (3) needs to be repeated, so that the energy spectrum diagnosis of the Thomson ion spectrometer is realized, and the high-precision proton absolute energy spectrum in a wide range is obtained.
The aiming method of the proton absolute energy spectrum measuring device can simultaneously realize the quick aiming of the Thomson ion spectrometer and the radiochromic membrane stack, and can detect whether the radiochromic membrane stack interferes with the diagnosis of the Thomson ion spectrometer.
The utility model has the advantages of it is following:
(1) the utility model discloses proton absolute energy spectrum measuring device, through the diagnosis of combination radiation discoloration diaphragm stack and thomson ion spectrometer, carry out contrastive analysis and data fitting to both measured data, can give the absolute energy spectrum that is higher than certain energy laser acceleration proton.
(2) The second collimation hole of the organic glass collimator is adopted to replace the first collimation hole (actual collimation hole) of the spectrometer collimator 3, aiming laser pointing can be observed in real time, the laser pointing adjustment is changed from blind adjustment to accurate adjustment, and rapid laser pointing aiming is realized; because of the whole encapsulation of thomson spectrometer, can't observe the pointing of aiming at the light path, and the actual collimation hole aperture of thomson spectrometer only has hundred microns magnitude moreover, and it is very big to wear out the collimation hole degree of difficulty with aiming light through blind accent. The change is the organic glass collimation hole that the aperture is 1mm in this embodiment, can observe to aim laser on the one hand directional, realizes quick laser directional regulation, and on the other hand, the actual collimation hole aperture of thomson spectrometer only has hundred microns orders of magnitude, can take place obvious diffraction effect, leads to aiming the light path precision poor, and the aperture that changes to 1mm is to aiming the finite hole effect of laser, can not take place obvious diffraction effect simultaneously again, consequently aims the light path and collimates more.
(3) Place the radiochromic diaphragm of a slice center trompil before the collimation hole, can detect the aiming effect, be convenient for confirm whether radiochromic diaphragm stack forms the interference to thomson ion spectrometer's diagnosis. During measurement, because the radiochromic diaphragm stack is very close to an experimental target, the work of the aiming target system can be influenced if the radiochromic diaphragm stack is directly placed at a diagnosis position before measurement. The radiochromic membrane stack is therefore moved out of the diagnostic position prior to measurement. And when the target is formally hit to be measured, the radiochromic membrane stack is moved into a diagnosis position. The diagnostic process thus involves an accurate reset of the radiochromic membrane stack. If the resetting is inaccurate, the analysis of the experimental result is influenced.
The embodiments in the present description are described in a progressive manner, each embodiment focuses on differences from other embodiments, and the same and similar parts among the embodiments are referred to each other.
The principle and the implementation of the present invention are explained herein by using specific examples, and the above description of the embodiments is only used to help understand the method and the core idea of the present invention; meanwhile, for the general technical personnel in the field, according to the idea of the present invention, there are changes in the concrete implementation and the application scope. In summary, the content of the present specification should not be construed as a limitation of the present invention.
Claims (9)
1. A proton absolute energy spectrum measuring apparatus, comprising: the Thomson ion spectrometer and the radiochromic membrane stack are sequentially arranged from the aiming laser emission end to the experimental target end; the center of the radiation color-changing membrane stack is provided with a central through hole; the axis of the central through hole is superposed with the axis of an inlet and outlet hole of the Thomson ion spectrometer; the Thomson ion spectrometer is used for receiving aiming laser and enabling the aiming laser to pass through a central through hole of the radiochromic membrane stack to reach an experimental target point; the experimental target is used for receiving experimental targeting laser and accelerating the experimental targeting laser to generate protons, and the protons are irradiated on the radiochromic membrane stack; the thomson ion spectrometer is also configured to receive protons that pass through a central through-hole of the radiochromic membrane stack.
2. The device of claim 1, wherein the thomson ion spectrometer comprises an imaging plate, a spectrometer electromagnetic assembly and a spectrometer collimator which are arranged in sequence from the aiming laser emission end to the experimental target end; the imaging plate and the spectrometer collimator are both connected with the spectrometer electromagnetic assembly; a first collimating hole is formed in the center of the spectrometer collimator; the axis of the central through hole coincides with the axis of the first collimating hole.
3. The device according to claim 1, wherein the radiochromic membrane stack comprises a group of radiochromic membranes and a metal shielding membrane stacked in a horizontal direction; the radiochromic diaphragm set comprises a plurality of layers of first radiochromic diaphragms which are stacked along the horizontal direction; the metal shielding diaphragm is arranged on one side far away from the Thomson ion spectrometer.
4. A proton absolute spectroscopy apparatus according to claim 2 wherein the diameter of the central through hole is greater than the diameter of the first collimating hole.
5. The apparatus according to claim 2, wherein the thomson ion spectrometer further comprises a second radiochromic diaphragm; the second radiochromic diaphragm is arranged at the front end of the spectrometer collimator and is positioned between the Thomson ion spectrometer and the radiochromic diaphragm stack; a diaphragm through hole is formed in the center of the second radiochromic diaphragm; the diameter of the diaphragm through hole is larger than that of the first collimating hole.
6. The apparatus according to claim 5, further comprising a collimated laser pointer; the aiming laser pen is used for emitting the aiming laser and enabling the aiming laser to enter the Thomson ion spectrometer.
7. The apparatus of claim 6, further comprising a first adjustment stage, a second adjustment stage, and a third adjustment stage; the Thomson ion spectrometer is arranged on the first adjusting platform, and the first adjusting platform is used for adjusting the lifting, the transverse translation, the rotation and the pitching of the Thomson ion spectrometer; the radiochromic membrane stack is arranged on the second adjusting platform, and the second adjusting platform is used for adjusting the translation and the lifting of the radiochromic membrane stack; the aiming laser pen is arranged on the third adjusting platform; the third adjusting platform is used for adjusting the position of the aiming laser pen.
8. The apparatus of claim 6, further comprising a plexiglas collimator; a second collimating hole is formed in the center of the organic glass collimator; the organic glass collimator is used for replacing the spectrometer collimator when aiming operation is carried out.
9. The apparatus according to claim 8, further comprising a collimator plate; the aiming piece is arranged at an experimental target point; the distance between the sighting piece and the radiochromic membrane stack is 5cm-10 cm.
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| GR01 | Patent grant | ||
| GR01 | Patent grant |